The force Fρ to affect a change in ψ is given by,
Fρ=−∂ψ∂x
This force act against the system and results in work done that is equal to a change in energy ψ. So, the resistance exerted by the system of a solitary particle on an external agent is given by,
Fi=−Fρ=∂ψ∂x
where Fi is the force exerted by the particle on an external agent. So,
Fi=−Fρ=−i√2mc2G.tanh(G√2mc2(x−xz))
The following diagram shows the interaction between two monopoles of positive Fi, ie (-Fρ)
The concentration of ψ between the two particles pushes them apart. And their interaction is thus repulsive.
In a similar way, the diagram below shows the interaction between two monopoles of −Fi, ie (+Fρ)
The depletion of ψ between the two particles pulls them together. And their interaction is thus attractive.
Both diagrams show Fρ, the force developed in previous posts, from an external agent affecting a change in ψ around the particle. Strictly speaking the force due to the particles are,
And the interaction of two dissimilar particles is,
If the interaction of two positive Fi is that of charges (repulsive, like charges repel) and the interaction of two −Fi is that of gravity particle (attractive, two masses attract), then the interaction of Fi and −Fi shown above, is attractive as though the charge has mass; the interaction between two masses is attractive.
If the interaction of +Fi is that of negative charges, then along the negative tc time dimension we have positive charges. Similarly, along −tg time dimension, anti-mass particles.
Negative and positive charges are matter/anti-matter pair, and mass and anti-mass are similarly matter/anti-matter pair.